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MOTION MOUNTAIN

LIGHT, CHARGES AND BRAINS - Motion Mountain

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80 2 the description of electromagnetic field evolution<br />

Field lines<br />

imagined as<br />

water flow<br />

paddle-wheel<br />

F I G U R E 46 Visualizing the curl of a vector field. Imagine the field to be flowing air and check whether<br />

the small paddle-wheel rotates; if it does, the local curl is non-zero. The direction of the curl is the<br />

direction of the paddle-wheel axis that yields the highest rotation velocity.<br />

Ref. 44<br />

Challenge 78 ny<br />

Ref. 45<br />

Challenge 79 ny<br />

step is the definition of the(magnetic)vector potential, which describes the momentum<br />

per charge that the field provides:<br />

A= p q . (34)<br />

When a charged particle moves through a magnetic potentialA(x), its momentum<br />

changes byqΔA; it changes by the difference between the potential values at the start<br />

and end points, multiplied by its charge. Owing to this definition, the vector potential<br />

has the property that<br />

B=∇×A=curlA (35)<br />

i.e., that the magnetic field is thecurl of the magnetic potential. In most other languages<br />

the curl is called therotation and abbreviated rot. To visualize what the curl or rotation<br />

is, imagine that the field vectors are the velocity vectors of flowing air. Now put a tiny<br />

paddle-wheelatapoint,asshowninFigure46.Ifitturns,thecurlisnon-zero.Therotation<br />

speedof the paddle-wheel is maximal for somedirection of theaxis; this maximal<br />

speeddefines boththemagnitude and thedirection of thecurl at thepoint. (Therighthandrule<br />

is implied.) For example, thecurl for the velocities of a rotating solid body is<br />

everywhere2ω, or twice the angular velocity.<br />

The vector potential for a long straight current-carryingwireisparalleltothewire;it<br />

hasthemagnitude<br />

A(r)=− μ 0I<br />

4π lnr r 0<br />

, (36)<br />

whichdependsontheradialdistancerfromthewireandanintegrationconstantr 0 .This<br />

expressionforthe vector potential, pictured in Figure 45, shows how the moving current<br />

produces a linear momentum in the (electro-)magnetic fieldaroundit. In thecaseof a<br />

solenoid,the vector potential ‘circulates’ around the solenoid.The magnitude obeys<br />

A(r)=− Φ 1<br />

4πr , (37)<br />

Motion Mountain – The Adventure of Physics copyright © Christoph Schiller June 1990–November 2015 free pdf file available at www.motionmountain.net

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